PHY862 Accelerator Systems Introduction to Accelerators Homework

Slides:



Advertisements
Similar presentations
Motion of a Charged Particle in a Magnetic Field
Advertisements

Applications of the Motion of Charged Particles in a Magnetic Field AP Physics C Montwood High School R. Casao.
P Spring 2003 L2Richard Kass Relativistic Kinematics In HEP the particles (e.g. protons, pions, electrons) we are concerned with are usually moving.
AS 4002 Star Formation & Plasma Astrophysics BACKGROUND: Maxwell’s Equations (mks) H (the magnetic field) and D (the electric displacement) to eliminate.
Particle Accelerators
Charged Particles in Electric and Magnetic Fields Motion of charged particles Lorentz Force Examples: cyclotron, mass spectrometer.
Homework due Monday. Use Compton scattering formula for Ch5 Q8 An electron volt (eV) is a unit of energy = work done moving an electron down one volt =
Prof. Reinisch, EEAS / Simple Collision Parameters (1) There are many different types of collisions taking place in a gas. They can be grouped.
EPPT M2 INTRODUCTION TO RELATIVITY K Young, Physics Department, CUHK  The Chinese University of Hong Kong.
1 Measuring masses and momenta u Measuring charged particle momenta. u Momentum and Special Relativity. u Kinetic energy in a simple accelerator. u Total.
PHY 1371Dr. Jie Zou1 Chapter 39 Relativity (Cont.)
I-4 Simple Electrostatic Fields Main Topics Relation of the Potential and Intensity The Gradient Electric Field Lines and Equipotential.
January 9, 2001Physics 8411 Space and time form a Lorentz four-vector. The spacetime point which describes an event in one inertial reference frame and.
Accelerator Physics  Basic Formalism  Linear Accelerators  Circular Accelerators  Magnets  Beam Optics  Our Accelerator Greg LeBlanc Lead Accelerator.
Magnetic Fields and Forces
Particle accelerators and detectors -Short Answers.
Lecture 5: Electron Scattering, continued... 18/9/2003 1
Basic Mathematics Rende Steerenberg BE/OP CERN Accelerator School Basic Accelerator Science & Technology at CERN 3 – 7 February 2014 – Chavannes de Bogis.
Centripetal force on charges in magnetic fields
Relativistic Kinetic Energy
Physics of Particle Accelerators Kalanand Mishra Department of Physics University of Cincinnati.
Accelerating Charge Through A Potential Difference.
Chapter 29 Magnetism Ferromagnetism
Chapter 26 Magnetism Poles – Location where the magnetic effect is the strongest –North pole – pole of a freely suspended magnet which points towards geographic.
Accelerator Physics with Relativity By Mark, Jack and Frances (Designing the LHC in an hour and a half)
General Physics II, Additional Questions, By/ T.A. Eleyan 1 Additional Questions Lec. 15,16.
Magnetism1 Review on Magnetism Chapter 28 Magnetism2 Refrigerators are attracted to magnets!
Eric Prebys, FNAL.  In terms of total charge and current  In terms of free charge an current USPAS, Knoxville, TN, January 20-31, 2013 Lecture 2 - Basic.
When charged particles move through magnetic fields, they experience a force, which deflects them Examples of such particles are electrons, protons, and.
Electric Potential Energy and the Electric Potential
Physics 121 Practice Problem Solutions 09 Magnetic Fields
Magnetic field Chapter 28.
System of Particles: Center-of-Mass
Monday, Jan. 31, 2005PHYS 3446, Spring 2005 Jae Yu 1 PHYS 3446 – Lecture #4 Monday, Jan. 31, 2005 Dr. Jae Yu 1.Lab Frame and Center of Mass Frame 2.Relativistic.
1 Electric Potential Reading: Chapter 29 Chapter 29.
Accelerated ions Contents: Electron Volts and accelerated ions.
1 Motion in Electric Fields SACE Stage 2 Physics.
Copyright © 2009 Pearson Education, Inc. E Determined from V.
Motion of Charges in Electric Fields. Electric Potential Difference.
AXEL-2017 Introduction to Particle Accelerators
Magnetic Fields and Forces
Special Theory of Relativity
Electrical Potential.
Relativistic Momentum
Charged Particles in Electric and Magnetic Fields
Chapter 25 Electric Potential.
How to calculate a dot product
Transformation of EM Fields
Magnetic Fields Contents: Overview What Produces Magnetic Field
Warm-up set 8 Question Answer:
IV . Electric ______________
Information Next lecture on Wednesday, 9/11/2013, will
Energy and momentum units in particle physics
Phys 102 – Lecture 4 Electric potential energy & work.
Chapter 29 Examples Examples 1, 6, 7.
Introduction to Accelerators
Magnetic Fields Chapter 26 Definition of B
Chapter 29 Electric Potential Reading: Chapter 29.
Physics 133 Electromagnetism
Unit 2 Particles and Waves Electric Fields and Movements of Charge
G. A. Krafft Jefferson Lab Old Dominion University Lecture 1
AXEL-2011 Introduction to Particle Accelerators
V (in Volts) = Potential EPE (in Joules) = Electric Potential Energy
Information Next lecture on Wednesday, 9/11/2013, will
RHIC Magnets for JLEIC Yuhong Zhang May 11, 2018.
PHYS 3446 – Lecture #4 Monday, Sept. 11, 2006 Dr. Jae Yu
Main Design Parameters RHIC Magnets for MEIC Ion Collider Ring
PHYS 1444 – Section 003 Lecture #3
Unit 2 Particles and Waves Electric Fields and Movements of Charge
Beam Synchronization in MEIC: The Problem, Scale and Prospect
Presentation transcript:

PHY862 Accelerator Systems Introduction to Accelerators Homework Peter N. Ostroumov Professor of Physics Michigan State University

Homework, p.1 What is the kinetic energy in units of both Joules and electron volts for an electron accelerated through a dc potential of 1 Megavolt? Find an expression for the fractional error when the nonrelativistic approximation for kinetic energy as a function of  is used. (a) At what values of  and  does the error in kinetic energy equal 1%? (b) To what kinetic energy does this correspond, for electrons and for protons? If the only nonzero components of the electromagnetic field in cylindrical coordinates are Er, Ez, and B, write the nonzero components of the Lorentz force for a particle of mass m and charge q moving along the z direction with velocity v. The rate of work done by a force F acting on a particle with velocity v is . Using the definition of the Lorentz force and the appropriate vector relationship, derive the expression for the rate of kinetic energy gain for a particle of charge q, and show that the magnetic force does not contribute. P.N. Ostroumov PHY862 "Aceclerator Systems" Fall 2018

Homework, p.2 Please answer the following questions for a proton traveling at a velocity of 0.9c. What is its momentum [GeV/c]? What is its kinetic energy [GeV]? What is its rigidity [T-m]? If this proton travels through a 1cm long magnet with a 1T field, by what angle will it be deflected [rad]? The Relativistic Heavy Ion Collider (RHIC) collides fully stripped gold ions (A=197, Z=79) at a total energy of E_coll=100 GeV/nucleon per beam. The circumference of each ring is 3834 m. Assume the rest mass of a gold ion is 197×0.93113 GeV. Calculate the revolution frequency of a particle at the injection energy of E_inj=10.5 GeV/nucleon, and at the storage energy of E_coll=100 GeV/nucleon. What is the change in revolution frequency for particles accelerated from E_inj to E_coll? If we assume that there are 192 identical dipoles per ring, each of length L= 10 m, what is the required dipole field in each at the collision energy of E coll? Read APS booklet “accelerators and beams” https://www.aps.org/units/dpb/news/edition4th.cfm P.N. Ostroumov PHY862 "Aceclerator Systems" Fall 2018